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NSR database version of June 30, 2015.

Search: Author = M.Horoi

Found 87 matches.

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2015NE03     Phys.Rev. C 91, 024309 (2015)

A.Neacsu, M.Horoi

Shell model studies of the 130Te neutrinoless double-β decay

NUCLEAR STRUCTURE 130Te, 130,136Xe, 136Ba; calculated levels, J, π, GT strengths for 130Te to 130I and 136Xe to 136Cs transitions. 128,130Te, 130,132Xe; calculated neutron and proton shell vacancies, B(E2). Shell model calculations using SVD effective Hamiltonian. Comparison with available experimental values.

RADIOACTIVITY 130Te, 136Xe(2β-); calculated GT strengths nuclear matrix elements (NME) for 2νββ and 0νββ decays for light and heavy neutrino exchanges. Shell model approach using a recently proposed effective Hamiltonian SVD, and jj55 model space. Comparison with calculations for double β decays of 48Ca, 76Ge, 82Se.

doi: 10.1103/PhysRevC.91.024309


2014BR22     Phys.Rev.Lett. 113, 262501 (2014)

B.A.Brown, M.Horoi, R.A.Senkov

Nuclear Structure Aspects of Neutrinoless Double-β Decay

RADIOACTIVITY 76Ge, 48Ca, 82Se(2β-); calculated nuclear matrix elements as sums of products over the intermediate nucleus with two less nucleons; deduced the importance of the ground state of intermediate nucleus.

doi: 10.1103/PhysRevLett.113.262501


2014HA06     Phys.Rev. C 89, 034315 (2014)

M.Haaranen, M.Horoi, J.Suhonen

Shell-model study of the 4th- and 6th-forbidden β-decay branches of 48Ca

RADIOACTIVITY 48Ca(β-), (2β-); calculated partial half-lives for 4th and 6th-forbidden β decays to 6+, 5+ and 4+ states in 48Sc. Competition between single β decay and 2νββ decay branches. Shell-model calculations using GXPF1A effective interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.034315


2014KW04     Phys.Rev. C 89, 045502 (2014)

A.A.Kwiatkowski, T.Brunner, J.D.Holt, A.Chaudhuri, U.Chowdhury, M.Eibach, J.Engel, A.T.Gallant, A.Grossheim, M.Horoi, A.Lennarz, T.D.Macdonald, M.R.Pearson, B.E.Schultz, M.C.Simon, R.A.Senkov, V.V.Simon, K.Zuber, J.Dilling

New determination of double-β-decay properties on 48Ca High-precision Qββ-value measurement and improved nuclear matrix element calculations

ATOMIC MASSES 48Ca, 48Ti; measured cyclotron-frequencies, resonances using TITAN system consisting of radio frequency quadrupole (RFQ) beam cooler and buncher, an electron beam ion trap (EBIT), and a Penning trap (MPET) at ISAC-TRIUMF facility; deduced Q value for double β decay of 48Ti. Comparison with previous measurements and atomic mass evaluations (AME-2003 and AME-2012).

RADIOACTIVITY 48Ca(2β-); measured precise Q-value using TITAN system at ISAC-TRIUMF facility; calculated ββ nuclear matrix element by including effects of levels outside the valence space in a shell-model; discussed case for a new experiment on double-beta decay of 48Ca.

doi: 10.1103/PhysRevC.89.045502


2014PR06     Nucl.Data Sheets 120, 112 (2014)

B.Pritychenko, M.Birch, M.Horoi, B.Singh

B(E2) Evaluation for 0+1 → 2+1 Transitions in Even-Even Nuclei

COMPILATION 46,48Ca, 46,48Ti, 70Zn, 70,76Ge, 76,80,82Se, 80,82,86Kr, 86Sr, 94,96Zr, 94,96,100Mo, 100,104Ru, 104,110Pd, 110,114,116Cd, 114,116,122,124Sn, 122,124,128,130Te, 128,130,134,136Xe, 134,136Ba; compiled evaluated B(E2) values, deformation parameters, first 2+ state energies for 2β-decay candidates.

doi: 10.1016/j.nds.2014.07.021


2014SA46     Phys.Lett. B 736, 137 (2014)

A.Sanetullaev, M.B.Tsang, W.G.Lynch, Jenny Lee, D.Bazin, K.P.Chan, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, A.M.Rogers, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, D.Shapira, W.A.Peters, C.Barbieri, M.Hjorth-Jensen, M.Horoi, T.Otsuka, T.Suzuki, Y.Utsuno

Neutron spectroscopic factors of 55Ni hole-states from image transfer reactions

NUCLEAR REACTIONS 1H(56Ni, d), E=37 MeV/nucleon; measured reaction products; deduced spectroscopic factors, J, π, σ(θ). Comparison with shell model calculations.

doi: 10.1016/j.physletb.2014.07.003
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2014SE10     Phys.Rev. C 89, 054304 (2014)

R.A.Sen'kov, M.Horoi, B.A.Brown

Neutrinoless double-β decay of 82Se in the shell model: Beyond the closure approximation

RADIOACTIVITY 82Se(2β-); calculated nuclear matrix elements for neutrinoless double-beta decay (0νββ). Shell-model techniques using CD-Bonn-, Miller-Spencer-, and AV18-based short-range correlation (SRC) methods. Comparison with other theoretical calculations. Relevance to SuperNEMO experiment.

doi: 10.1103/PhysRevC.89.054304


2014SE21     Phys.Rev. C 90, 051301 (2014)

R.A.Senkov, M.Horoi

Accurate shell-model nuclear matrix elements for neutrinoless double-β decay

RADIOACTIVITY 76Ge(2β-); calculated nuclear matrix elements (NMEs), and average closure energies for neutrinoless double-β decay using realistic shell-model approach beyond closure approximation. 44,46,48Ca, 76Ge, 82Ge(2β-); calculated optimal closure energies for GXPF1A, FPD6, and KB3G for Ca and JUN45 for Ge and Se isotopes.

doi: 10.1103/PhysRevC.90.051301


2013BO19     Comput.Phys.Commun. 184, 085101 (2013)

S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild

Computational nuclear quantum many-body problem: The UNEDF project

NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data.

NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.

doi: 10.1016/j.cpc.2013.05.020


2013HO03     Phys.Rev. C 87, 014320 (2013)

M.Horoi

Shell model analysis of competing contributions to the double-β decay of 48Ca

RADIOACTIVITY 48Ca(2β-); calculated two-neutrino and neutrinoless 2β- nuclear matrix elements, T1/2, prediction for transition to the first excited 0+ state using shell-model calculations.

doi: 10.1103/PhysRevC.87.014320


2013HO11     Phys.Rev.Lett. 110, 222502 (2013)

M.Horoi, B.A.Brown

Shell-Model Analysis of the 136Xe Double Beta Decay Nuclear Matrix Elements

RADIOACTIVITY 136Xe(2β-); calculated neutrinoless mode nuclear matrix elements; deduced importance of nuclear orbitals necessary for a good description of the Gamow-Teller strength. Shell model analysis, comparison with available data.

doi: 10.1103/PhysRevLett.110.222502


2013LU10     Phys.Rev. C 88, 017604 (2013)

F.Lu, J.Lee, M.B.Tsang, D.Bazin, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, W.G.Lynch, A.M.Rogers, A.Sanetullaev, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, M.Horoi, Y.L.Ye

Neutron-hole states in 45Ar from 1H(46Ar, d)45Ar reactions

NUCLEAR REACTIONS 1H(46Ar, d), E=33 MeV/nucleon; measured E(d), I(d), σ(θ). Radioactive secondary beam of 46Ar produced in the Coupled Cyclotron facility at NSCL. 45Ar; deduced levels, J, π, L-transfer, spectroscopic factors. ADWA analysis. Comparison with spectroscopic factors determined in 2H(44Ar, p)45Ar reaction, and with shell-model calculations.

doi: 10.1103/PhysRevC.88.017604
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2013SE22     Phys.Rev. C 88, 064312 (2013)

R.A.Sen'kov, M.Horoi

Neutrinoless doubleβ in the shell model: Closure versus nonclosure approximation

RADIOACTIVITY 48Ca(2β-); calculated the 0νββ nuclear matrix elements (NMEs) using closure approximation, a nonclosure approach, and a combined new method within shell model. 44,46Ca; calculated closure NME for fictitious 0νββ decay.

doi: 10.1103/PhysRevC.88.064312


2012BA33     Phys.Rev. C 86, 015806 (2012), Erratum Phys.Rev. C 86, 039901 (2012)

A.Banu, F.Carstoiu, N.L.Achouri, W.N.Catford, M.Chartier, B.Fernandez-Dominguez, M.Horoi, B.Laurent, N.A.Orr, S.Paschalis, N.Patterson, B.Pietras, B.T.Roeder, P.Roussel-Chomaz, J.S.Thomas, L.Trache, R.E.Tribble

One-proton breakup of 24Si and the 23Al(p, γ)24Si reaction in type I x-ray bursts

NUCLEAR REACTIONS 12C(24Si, 23Al), [24Si secondary beam from C(32S, X), E=95 MeV/nucleon primary reaction], E=61 MeV/nucleon; measured fragment spectra, σ, inclusive longitudinal momentum distribution, time-of-flight of 23Al fragments using SPEG spectrograph at GANIL; deduced spectroscopic factors, asymptotic normalization coefficient (ANC). Glauber-type analysis. Comparison with large-scale shell model calculations. 23Al(p, γ)24Si, E<1 MeV; deduced stellar reaction rates. Discussed astrophysical significance of 23Al(p, γ)24Si in type I x-ray bursts (XRB) nucleosynthesis. Waiting-point nuclei and relevance to 22Na abundance and sequential 2p capture on 22Mg at high temperature.

doi: 10.1103/PhysRevC.86.015806
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2012BA46     J.Phys.:Conf.Ser. 337, 012059 (2012)

A.Banu, F.Carstoiu, W.N.Catford, B.Fernandez-Dominguez, M.Horoi, N.A.Orr, B.T.Roeder, P.Roussel-Chomaz, L.Trache, R.E.Tribble

Direct radiative proton capture 23Al(p, γ)24Si studied via one-proton nuclear breakup of 24Si

NUCLEAR REACTIONS 12C(24Si, p23Al), E=20-60 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin, reaction products using SPEG energy-loss spectrometer; deduced 23Al momentum distribution; calculated 23Al momentum distribution using Glauber-type approach.

doi: 10.1088/1742-6596/337/1/012059


2012DI04     Phys.Rev. C 85, 034311 (2012)

E.S.Diffenderfer, L.T.Baby, D.Santiago-Gonzalez, N.Ahsan, A.Rojas, A.Volya, I.Wiedenhover, A.H.Wuosmaa, M.P.Carpenter, R.V.F.Janssens, C.J.Lister, M.Devlin, D.G.Sarantites, L.G.Sobotka, Y.Utsuno, M.Horoi

High-spin spectrum of 24Mg studied through multiparticle angular correlations

NUCLEAR REACTIONS 12C(16O, α)24Mg, E=62, 68 MeV; measured Eα, Iα, αγ-coin, αγ(θ), αγγ(θ) using Gammasphere array. Experiments carried out at ANL and FSU facilities. 24Mg; deduced levels, J, π, configurations. Comparison with previous studies and shell model calculations.

doi: 10.1103/PhysRevC.85.034311
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2012NE11     Phys.Rev. C 86, 067304 (2012)

A.Neacsu, S.Stoica, M.Horoi

Fast, efficient calculations of the two-body matrix elements of the transition operators for neutrinoless double-β decay

RADIOACTIVITY 48Ca, 82Se(2β-); calculated two-body matrix elements (TBME) of neutrinoless double beta (0νββ) decay transition operator using a new, and fast algorithm.

doi: 10.1103/PhysRevC.86.067304


2012PR08     At.Data Nucl.Data Tables 98, 798 (2012)

B.Pritychenko, J.Choquette, M.Horoi, B.Karamy, B.Singh

An update of the B(E2) evaluation for 0+1 → 2+1 transitions in even-even nuclei near N ∼ Z ∼ 28

COMPILATION 46,48,50,52,54,56,58,60,62,64Cr, 48,50,52,54,56,58,60,62,64,66,68Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 60,62,64,66,68,70,72,74,76,78,80Zn; compiled evaluated and experimental B(E2) values and transition energies.

NUCLEAR STRUCTURE 46,48,50,52,54,56,58,60,62Cr, 50,52,54,56,58,60,62,64Fe, 54,56,58,60,62,64,66,68,70,72,74,76Ni, 62,64,66,68,70,72,74,76,78Zn; calculated B(E2) values, transition energies. Nuclear shell model, GXPF1A and JUN45 effective interactions.

doi: 10.1016/j.adt.2012.06.004


2011BA27     Phys.Rev. C 84, 015803 (2011)

A.Banu, L.Trache, F.Carstoiu, N.L.Achouri, A.Bonaccorso, W.N.Catford, M.Chartier, M.Dimmock, B.Fernandez-Dominguez, M.Freer, L.Gaudefroy, M.Horoi, M.Labiche, B.Laurent, R.C.Lemmon, F.Negoita, N.A.Orr, S.Paschalis, N.Patterson, E.S.Paul, M.Petri, B.Pietras, B.T.Roeder, F.Rotaru, P.Roussel-Chomaz, E.Simmons, J.S.Thomas, R.E.Tribble

Structure of 23Al from the one-proton breakup reaction and astrophysical implications

NUCLEAR REACTIONS 12C(23Al, 22Mg), [23Al secondary beam from C(32S, X)E=95 MeV/nucleon primary reaction], E=57 MeV/nucleon; measured fragment spectra, inclusive and exclusive longitudinal momentum distributions, and widths, Eγ, (fragment)γ-coin. 22Mg; deduced levels, J, π, σ, spectroscopic factors, asymptotic normalization coefficients. 23Al; deduced g.s. Jπ, configuration mixing. Comparison with Glauber and large-scale shell model calculations. 22Mg(p, γ)23Al, E<1 MeV; deduced stellar reaction rates; discussed astrophysical significance of 22Na nucleosynthesis in ONe novae.

doi: 10.1103/PhysRevC.84.015803
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2011GA22     Phys.Rev. C 83, 057303 (2011)

Z.-C.Gao, M.Horoi, Y.S.Chen, Y.J.Chen, Tuya

Can one identify the intrinsic structure of the yrast states in 48Cr after the backbending?

NUCLEAR STRUCTURE 48Cr; calculated levels, J, π, B(E2), configurations for yrast states using projected configuration interaction (PCI) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.057303


2010HO02     Phys.Rev. C 81, 024321 (2010)

M.Horoi, S.Stoica

Shell model analysis of the neutrinoless double-β decay of 48Ca

RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix elements for neutrinoless double-β decay using large-scale shell model.

NUCLEAR STRUCTURE 48Ca, 48Ti; calculated neutron and proton occupation probabilities, and nuclear matrix elements for double-β decay using large-scale shell model.

doi: 10.1103/PhysRevC.81.024321


2010HO05     Phys.Rev. C 81, 034306 (2010)

M.Horoi, V.Zelevinsky

Random interactions explore the nuclear landscape: Predominance of prolate nuclear deformations

doi: 10.1103/PhysRevC.81.034306


2010PE15     Phys.Rev. C 82, 064305 (2010)

S.M.Perez, W.A.Richter, B.A.Brown, M.Horoi

Magnetic moments of T=3/2 mirror pairs

NUCLEAR MOMENTS 43V, 43Ca, 45Sc, 45Cr, 47Mn, 47Ti, 49Fe, 49V, 51Co, 51Cr, 53Ni, 53Mn; analyzed magnetic moments, γp and γn values of T=3/2 proton-rich nuclei in fp shell by using experimental values for their neutron-rich mirror nuclei. 19Na, 19O, 21F, 21Mg, 23Al, 23Ne, 25Na, 25Si, 27P, 27Mg, 29Al, 29S, 31Cl, 31Si, 33P, 33Ar, 35K, 35S, 37Cl, 37Ca; analyzed gp and γn values of T=3/2 mirror nuclei in sd shell. Shell model calculations.

doi: 10.1103/PhysRevC.82.064305


2010SC20     Europhys.Lett. 91, 52001 (2010)

M.Scott, M.Horoi

Improved accuracy moments method for spin-dependent shell model nuclear level densities

NUCLEAR STRUCTURE 48,50Ti, 50,52Cr, 64Ge; calculated nuclear level densities, positive- and negative-parity states.

doi: 10.1209/0295-5075/91/52001


2010SE09     Phys.Rev. C 82, 024304 (2010)

R.A.Senkov, M.Horoi

High-performance algorithm to calculate spin- and parity-dependent nuclear level densities

NUCLEAR STRUCTURE 28Si, 52Fe, 52Cr, 60Zn, 64Ge, 68Se, 70Br; calculated spin and parity dependent shell model nuclear level density using moments method in the proton-neutron formalism. Comparisons with exact shell-model calculations. Calculations performed on FRANKLIN supercomputer.

doi: 10.1103/PhysRevC.82.024304


2009GA03     Phys.Rev. C 79, 014311 (2009)

Z.-C.Gao, M.Horoi

Angular momentum projected configuration interaction with realistic Hamiltonians

NUCLEAR STRUCTURE 28Si; calculated ground-state energies. 20Ne, 24Mg, 28Si, 36Ar; calculated deformation HF energies. 24Mg, 28Si, 48Cr, 56Ni; calculated quadrupole moments, B(E2). 24Mg, 28Si, 48Cr; calculated levels, J, π. 52Fe, 56Ni; calculated yrast band energies using full configuration interaction method.in sd-pf shell space.

doi: 10.1103/PhysRevC.79.014311


2009GA29     Phys.Rev. C 80, 034325 (2009)

Z.-C.Gao, M.Horoi, Y.S.Chen

Improved basis selection for the projected configuration interaction method applied to medium-heavy nuclei

NUCLEAR STRUCTURE 56Ni, 68,70,76Se, 76Ge; calculated level energies using Projection Configuration Interaction (PCI) and full configuration interaction (CI) approaches. 76Ge, 76Se; calculated low-lying 0+ states.

doi: 10.1103/PhysRevC.80.034325


2009HI08     Phys.Rev. C 80, 014313 (2009)

G.W.Hitt, R.G.T.Zegers, Sam M.Austin, D.Bazin, A.Gade, D.Galaviz, C.J.Guess, M.Horoi, M.E.Howard, W.D.M.Rae, Y.Shimbara, E.E.Smith, C.Tur

Gamow-Teller transitions to 64Cu measured with the 64Zn(t, 3He) reaction

NUCLEAR REACTIONS 64Zn(t, 3He), E=115 MeV/nucleon; measured particle spectra, σ(θ) and Gamow-Teller strength distributions; deduced electron capture rate on 64Zn as a function of stellar temperature. Comparison with shell model calculations and experimental data from 64Zn(d, 2He) reaction.

doi: 10.1103/PhysRevC.80.014313
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1721.
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2009LE14     Phys.Rev. C 79, 054611 (2009)

J.Lee, M.B.Tsang, W.G.Lynch, M.Horoi, S.C.Su

Neutron spectroscopic factors of Ni isotopes from transfer reactions

NUCLEAR REACTIONS 58,60,61,62,64Ni(d, p), (p, d), E not given; analyzed experimental angular distributions using adiabatic distorted wave approximation (ADWA). 57,58,59,60,61,62,63,64Ni; deduced spectroscopic factors for ground and excited states. Comparison with large basis shell-model calculations.

doi: 10.1103/PhysRevC.79.054611


2009TS01     Phys.Rev.Lett. 102, 062501 (2009)

M.B.Tsang, J.Lee, S.C.Su, J.Y.Dai, M.Horoi, H.Liu, W.G.Lynch, S.Warren

Survey of Excited State Neutron Spectroscopic Factors for Z = 8-28 Nuclei

NUCLEAR STRUCTURE 17,18O, 21Ne, 24Na, 26,27Mg, 29,30,31Si, 33,35S, 41,43,45,47,49Ca, 47,49,51Ti, 51,53,55Cr, 57,59,61,62,63,65Ni; calculated excited state neutron spectroscopic factors.

doi: 10.1103/PhysRevLett.102.062501


2008GO19     Phys.Rev.Lett. 101, 052501 (2008)

J.R.Gour, M.Horoi, P.Piecuch, B.A.Brown

Coupled-Cluster and Configuration-Interaction Calculations for Odd-A Heavy Nuclei

NUCLEAR STRUCTURE 55,57Ni; calculated binding energies, and low-lying level energies using Coupled-Cluster and Configuration-Interaction.

doi: 10.1103/PhysRevLett.101.052501


2008MA01     Phys.Rev. C 77, 014313 (2008)

P.F.Mantica, R.Broda, H.L.Crawford, A.Damaske, B.Fornal, A.A.Hecht, C.Hoffman, M.Horoi, N.Hoteling, R.V.F.Janssens, J.Pereira, J.S.Pinter, J.B.Stoker, S.L.Tabor, T.Sumikama, W.B.Walters, X.Wang, S.Zhu

β decay of neutron-rich 53-56Ca

RADIOACTIVITY 53,54,55,56Ca(β-) [from 9Be(76Ge, X), E=140 MeV/nucleon; measured Eγ, Iγ, βγ-coin, half-lives. 54Ca; deduced Iβ, logft. 54Sc; levels, J, π, half-lives, B(M1), B(E2), comparison with calculations.

NUCLEAR REACTIONS 9Be(76Ge, X)49Cl/50Ar/51Ar/52K/53K/54K/53Ca/54Ca/55Ca/56Ca/55Sc/56Sc/57Sc/57Ti/58Ti/59Ti/60V, E=140 MeV/nucleon; measured reaction yields.

doi: 10.1103/PhysRevC.77.014313
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2008PE13     Phys.Rev. C 77, 064311 (2008)

S.M.Perez, W.A.Richter, B.A.Brown, M.Horoi

Correlations between magnetic moments and β decays of mirror nuclei

NUCLEAR STRUCTURE 11B, 11,13C, 13,15N, 15,17O, 17,19F, 19,21Ne, 21,23Na, 23,25Mg, 25,27Al, 27,29Si, 29,31P, 31,33S, 33,35Cl, 35,37Ar, 37,39K, 39,41Ca, 41,43Sc, 43,45Ti, 45,47V, 47,49Cr, 49,51Mn, 51,53Fe, 53,55Co, 55,57Ni, 57Cu; calculated magnetic moments, β-decay half-lives, gyromagnetic ratios.

doi: 10.1103/PhysRevC.77.064311


2007CA35     Phys.Lett. B 652, 169 (2007); Addendum Phys.Lett. B 656, 272 (2007)

C.M.Campbell, N.Aoi, D.Bazin, M.D.Bowen, B.A.Brown, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, M.Horoi, S.Kanno, T.Motobayashi, L.A.Riley, H.Sagawa, H.Sakurai, K.Starosta, H.Suzuki, S.Takeuchi, J.R.Terry, K.Yoneda, H.Zwahlen

Quadrupole collectivity in silicon isotopes approaching neutron number N=28

NUCLEAR REACTIONS 1H(36Si, 36Si'), E < 140 MeV/nucleon; 1H(38Si, 38Si'), E < 140 MeV/nucleon; 1H(40Si, 40Si'), E < 140 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coinc, inelastic proton scattering cross sections. 36,38,40Si deduced quadrupole deformation parameters.

doi: 10.1016/j.physletb.2007.07.005
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2007HO05     Phys.Rev.Lett. 98, 112501 (2007)

M.Horoi, J.R.Gour, M.Wloch, M.D.Lodriguito, B.A.Brown, P.Piecuch

Coupled-Cluster and Configuration-Interaction Calculations for Heavy Nuclei

NUCLEAR STRUCTURE 56Ni; calculated level energies, J, π, configurations. Comparison of coupled-cluster and configuration-interaction results.

doi: 10.1103/PhysRevLett.98.112501


2007HO07     Phys.Rev. C 75, 034303 (2007)

M.Horoi, S.Stoica, B.A.Brown

Shell-model calculations of two-neutrino double-β decay rates of 48Ca with the GXPF1A interaction

NUCLEAR STRUCTURE 48Ca; calculated 2νββ-decay matrix elements, T1/2 for decay to ground and excited states. Shell model approach.

RADIOACTIVITY 48Ca(2β-); calculated 2νββ-decay matrix elements, T1/2 for decay to ground and excited states. Shell model approach.

doi: 10.1103/PhysRevC.75.034303


2007HO10     Phys.Rev. C 75, 054303 (2007)

M.Horoi, V.Zelevinsky

Pairing phase transitions in nuclear wave functions

NUCLEAR STRUCTURE 24Mg, 28Si; calculated pairing correlator in sd shell model.

doi: 10.1103/PhysRevC.75.054303


2007HO12     Phys.Rev.Lett. 98, 262503 (2007)

M.Horoi, V.Zelevinsky

Exact Removal of the Center-of-Mass Spurious States from Level Densities

doi: 10.1103/PhysRevLett.98.262503


2007LI84     Eur.Phys.J. Special Topics 150, 135 (2007)

S.N.Liddick, P.F.Mantica, R.V.F.Janssens, B.A.Brown, M.P.Carpenter, A.D.Davies, M.Honma, M.Horoi, T.Mizusaki, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking

Beta-delayed γ-ray studies of πf7/2 - νpf shell nuclei

doi: 10.1140/epjst/e2007-00286-4


2007ST16     Phys.Rev.Lett. 99, 042503 (2007)

K.Starosta, A.Dewald, A.Dunomes, P.Adrich, A.M.Amthor, T.Baumann, D.Bazin, M.Bowen, B.A.Brown, A.Chester, A.Gade, D.Galaviz, T.Glasmacher, T.Ginter, M.Hausmann, M.Horoi, J.Jolie, B.Melon, D.Miller, V.Moeller, R.P.Norris, T.Pissulla, M.Portillo, W.Rother, Y.Shimbara, A.Stolz, C.Vaman, P.Voss, D.Weisshaar, V.Zelevinsky

Shape and Structure of N=Z 64Ge: Electromagnetic Transition Rates from the Application of the Recoil Distance Method to a Knockout Reaction

NUCLEAR REACTIONS 93Nb(65Ge, n), (63Zn, n), E not given; measured Eγ, Iγ and transition rates using recoil distance method. 64Ge, 62Zn deduced B(E2) and lifetimes.

doi: 10.1103/PhysRevLett.99.042503
Data from this article have been entered in the XUNDL database. For more information, click here.


2007VA22     Phys.Rev.Lett. 99, 162501 (2007)

C.Vaman, C.Andreoiu, D.Bazin, A.Becerril, B.A.Brown, C.M.Campbell, A.Chester, J.M.Cook, D.C.Dinca, A.Gade, D.Galaviz, T.Glasmacher, M.Hjorth-Jensen, M.Horoi, D.Miller, V.Moeller, W.F.Mueller, A.Schiller, K.Starosta, A.Stolz, J.R.Terry, A.Volya, V.Zelevinsky, H.Zwahlen

Z=50 Shell Gap near 100Sn from Intermediate-Energy Coulomb Excitations in Even-Mass 106-112Sn Isotopes

NUCLEAR REACTIONS 197Au(106Sn, 106Sn'), (108Sn, 108Sn'), (110Sn, 110sn'), (112Sn, 112Sn'), E=78-81 MeV; measured Eγ, Iγ, (particle)γ-coinc from projectile coulomb excitation. 106,108,110,112Sn deduced B(E2).

doi: 10.1103/PhysRevLett.99.162501
Data from this article have been entered in the XUNDL database. For more information, click here.


2006CA26     Phys.Rev.Lett. 97, 112501 (2006)

C.M.Campbell, N.Aoi, D.Bazin, M.D.Bowen, B.A.Brown, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, M.Horoi, S.Kanno, T.Motobayashi, W.F.Mueller, H.Sakurai, K.Starosta, H.Suzuki, S.Takeuchi, J.R.Terry, K.Yoneda, H.Zwahlen

Measurement of Excited States in 40Si and Evidence for Weakening of the N = 28 Shell Gap

NUCLEAR REACTIONS 1H(40Si, 40Si'), (42P, 40SiX), E ≈ 80 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 40Si deduced excited states energies. Comparison with model predictions.

doi: 10.1103/PhysRevLett.97.112501
Data from this article have been entered in the XUNDL database. For more information, click here.


2006FO13     Phys.Rev. C 74, 034308 (2006)

N.Fotiades, A.F.Lisetskiy, J.A.Cizewski, R.Krucken, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, J.A.Becker, B.A.Brown, M.Horoi, W.Younes

First observation of high-spin states in 83Se

NUCLEAR REACTIONS 208Pb(18O, F)83Se/138Ba/139Ba/140Ba, E=91 MeV; measured Eγ, Iγ, γγ-coin. 83Se deduced high-spin levels, J, π, configurations. Gammasphere array.

doi: 10.1103/PhysRevC.74.034308
Data from this article have been entered in the XUNDL database. For more information, click here.


2006GA31     Phys.Rev. C 74, 034322 (2006)

A.Gade, B.A.Brown, D.Bazin, C.M.Campbell, J.A.Church, D.C.Dinca, J.Enders, T.Glasmacher, M.Horoi, Z.Hu, K.W.Kemper, W.F.Mueller, T.Otsuka, L.A.Riley, B.T.Roeder, T.Suzuki, J.R.Terry, K.L.Yurkewicz, H.Zwahlen

Evolution of the E(1/2+1) - E(3/2+1) energy spacing in odd-mass K, Cl, and P isotopes for N = 20-28

NUCLEAR REACTIONS H, C(46Ar, X)43Cl/45Cl, E=76.4 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin. 45Cl deduced level energy.

NUCLEAR STRUCTURE 35,37,39,41,43P, 37,39,41,43,45Cl, 39,41,43,45,47K; analyzed level energies, splitting.

doi: 10.1103/PhysRevC.74.034322
Data from this article have been entered in the XUNDL database. For more information, click here.


2006GA35     Phys.Rev. C 74, 047302 (2006)

A.Gade, R.V.F.Janssens, D.Bazin, B.A.Brown, C.M.Campbell, M.P.Carpenter, J.M.Cook, A.N.Deacon, D.-C.Dinca, S.J.Freeman, T.Glasmacher, M.Horoi, B.P.Kay, P.F.Mantica, W.F.Mueller, J.R.Terry, J.A.Tostevin, S.Zhu

One-neutron knockout in the vicinity of the N = 32 sub-shell closure: 9Be(57Cr, 56Cr+γ)X

NUCLEAR REACTIONS 9Be(57Cr, 56CrX), E=77 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin, parallel momentum distribution; deduced σ. 56Cr deduced levels, spectroscopic factors.

doi: 10.1103/PhysRevC.74.047302
Data from this article have been entered in the XUNDL database. For more information, click here.


2006HO07     Phys.Rev. C 73, 061305 (2006); Erratum Phys.Rev. C 74, 059904 (2006)

M.Horoi, B.A.Brown, T.Otsuka, M.Honma, T.Mizusaki

Shell model analysis of the 56Ni spectrum in the full pf model space

NUCLEAR STRUCTURE 56Ni; calculated levels, J, π, B(E2), rotational bands. Shell model, comparison with data.

doi: 10.1103/PhysRevC.73.061305


2006HO10     Chem.Phys.Lett. 427, 147 (2006)

M.Horoi, K.A.Jackson

Signature of shape transition and shape coexistence in mesoscopic systems

NUCLEAR STRUCTURE Sm; analyzed binding energies, shape transition and shape coexistence effects.

doi: 10.1016/j.cplett.2006.06.017


2006LI15     Phys.Rev. C 73, 044322 (2006)

S.N.Liddick, P.F.Mantica, B.A.Brown, M.P.Carpenter, A.D.Davies, M.Horoi, R.V.F.Janssens, A.C.Morton, W.F.Mueller, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking

Half-life and spin of 60Mng

RADIOACTIVITY 60Cr, 60Mn(β-) [from Be(86Kr, X) and subsequent decay]; measured β-delayed Eγ, Iγ, T1/2; deduced log ft. 60Fe, 60Mn deduced levels J, π, configurations, β-feeding intensities. Comparison with shell model predictions.

doi: 10.1103/PhysRevC.73.044322
Data from this article have been entered in the XUNDL database. For more information, click here.


2006WA18     Phys.Rev. C 74, 014605 (2006)

R.E.Warner, F.Carstoiu, J.A.Brown, F.D.Becchetti, D.A.Roberts, B.Davids, A.Galonsky, R.M.Ronningen, M.Steiner, M.Horoi, J.J.Kolata, A.Nadasen, C.Samanta, J.Schwarzenberg, K.Subotic

Reaction and proton-removal cross sections of 6Li, 7Be, 10B, 9, 10, 11C, 12N, 13, 15O, and 17Ne on Si at 15 to 53 MeV/nucleon

NUCLEAR REACTIONS Si(6Li, X), (7Be, X), (10B, X), (9C, X), (10C, X), (11C, X), (12N, X), (13O, X), (15O, X), (17Ne, X), E=15-53 MeV/nucleon; measured reaction and proton-removal σ. 6Li, 7Be, 10B, 9,10,11C, 12N, 13,15O, 17Ne deduced radii. Comparison with Glauber model predictions.

doi: 10.1103/PhysRevC.74.014605
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1445.


2005AS04     Phys.Rev. C 72, 024314 (2005)

N.I.Ashwood, M.Freer, D.J.Millener, N.A.Orr, F.Carstoiu, S.Ahmed, J.C.Angelique, V.Bouchat, W.N.Catford, N.M.Clarke, N.Curtis, F.Hanappe, M.Horoi, Y.Kerckx, J.L.Lecouey, F.M.Marques, T.Materna, G.Normand, S.Pain, N.Soic, C.Timis, A.Unshakova, V.A.Ziman

High-energy two-neutron removal from 10Be

NUCLEAR REACTIONS 12C(10Be, 2α), (10Be, n2α), E=30 MeV/nucleon; measured En, Eα, relative energy spectra, σ(E). 8,9Be deduced levels, J, π. Kinematically complete measurement.

doi: 10.1103/PhysRevC.72.024314
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1402.


2005HO23     Nucl.Phys. A758, 138c (2005)

M.Horoi

Can one measure the temperature dependence of the fusion reaction rates?

NUCLEAR REACTIONS 2H(t, α), 1H(7Li, α), 7Li(p, α), E=low; calculated enhancement factors vs temperature for astrophysical reaction rates.

doi: 10.1016/j.nuclphysa.2005.05.028


2005HO24     Nucl.Phys. A758, 142c (2005)

M.Horoi, M.Ghita, V.Zelevinsky

Comparison of approaches for spin- and parity-dependent shell model nuclear level density

NUCLEAR STRUCTURE 28Si; calculated spin- and parity-dependent shell model level densities. Several approaches compared.

doi: 10.1016/j.nuclphysa.2005.05.029


2005LI53     Phys.Rev. C 72, 054321 (2005)

S.N.Liddick, P.F.Mantica, R.Broda, B.A.Brown, M.P.Carpenter, A.D.Davies, B.Fornal, M.Horoi, R.V.F.Janssens, A.C.Morton, W.F.Mueller, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking

β-decay of odd-A 57Ti and 59V

RADIOACTIVITY 57Ti, 59V, 59Cr(β-) [from Be(86Kr, X)]; measured β-delayed Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 57V, 59Cr, 59Mn deduced levels, β-feeding intensities, deformation. Comparison with shell-model predictions.

doi: 10.1103/PhysRevC.72.054321
Data from this article have been entered in the XUNDL database. For more information, click here.


2005LI54     Eur.Phys.J. A 25, Supplement 1, 95 (2005)

A.F.Lisetskiy, B.A.Brown, M.Horoi

Exotic nuclei near 78Ni in a shell model approach

NUCLEAR STRUCTURE 70,72,74,76Ni, 92Mo, 94Ru, 96Pd, 98Cd; calculated B(E2). 57,59,61,63,65,67,69,71,73,75,77,79Cu; calculated level energies. Shell model, comparison with data.

doi: 10.1140/epjad/i2005-06-158-1


2004HO10     Phys.Rev. C 69, 041307 (2004)

M.Horoi, M.Ghita, V.Zelevinsky

Fixed spin and parity nuclear level density for restricted shell model configurations

doi: 10.1103/PhysRevC.69.041307


2004HO12     J.Phys.(London) G30, 945 (2004)

M.Horoi

Scaling behaviour in cluster decay

RADIOACTIVITY 224Th(16O); 224Th, 221Ra, 222,223Ac(14C); 221Ra, 222Ac(12C); 223Ac(15N); calculated cluster decay T1/2, Q-values, scaling behaviour.

doi: 10.1088/0954-3899/30/7/010


2004LI64     Phys.Rev. C 70, 044314 (2004)

A.F.Lisetskiy, B.A.Brown, M.Horoi, H.Grawe

New T=1 effective interactions for the f5/2 p3/2 p1/2 g9/2 model space: Implications for valence-mirror symmetry and seniority isomers

NUCLEAR STRUCTURE 58,60,62,64,66,68,70,72,74,76Ni, 80Zn, 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru, 96Pd, 98Cd; calculated level energies. 70,72,74,76Ni, 92Mo, 94Ru, 96Pd, 98Cd; calculated transitions B(E2). New T=1 effective interactions. Comparisons with data.

doi: 10.1103/PhysRevC.70.044314


2004LI75     Phys.Rev. C 70, 064303 (2004)

S.N.Liddick, P.F.Mantica, R.Broda, B.A.Brown, M.P.Carpenter, A.D.Davies, B.Fornal, T.Glasmacher, D.E.Groh, M.Honma, M.Horoi, R.V.F.Janssens, T.Mizusaki, D.J.Morrissey, A.C.Morton, W.F.Mueller, T.Otsuka, J.Pavan, H.Schatz, A.Stolz, S.L.Tabor, B.E.Tomlin, M.Wiedeking

Development of shell closures at N = 32, 34. I. β decay of neutron-rich Sc isotopes

RADIOACTIVITY 54,55,56Sc(β-) [from Be(86Kr, X)]; measured Eβ, Eγ, βγ-coin, T1/2. 54,55,56Ti deduced levels, J, π, configurations. Comparison with model predictions.

doi: 10.1103/PhysRevC.70.064303
Data from this article have been entered in the XUNDL database. For more information, click here.


2003HO04     Phys.Rev. C 67, 034303 (2003)

M.Horoi, B.A.Brown, V.Zelevinsky

Exponential convergence method: Nonyrast states, occupation numbers, and a shell-model description of the superdeformed band in 56Ni

NUCLEAR STRUCTURE 52Cr, 56Ni; calculated single-particle configurations. 56Ni deduced superdeformed band features. Exponential convergence method.

doi: 10.1103/PhysRevC.67.034303


2003HO08     Phys.Rev. C 67, 054309 (2003)

M.Horoi, J.Kaiser, V.Zelevinsky

Spin- and parity-dependent nuclear level densities and the exponential convergence method

doi: 10.1103/PhysRevC.67.054309


2003HO18     Nucl.Phys. A718, 502c (2003)

M.Horoi, R.Jora, V.Zelevinsky, A.St.J.Murphy, R.N.Boyd, T.Rauscher

The 45V(p, γ) thermonuclear reaction rate relevant to 44Ti production rate in core-collapsed supernovae: a shell model analysis

NUCLEAR REACTIONS 45V(p, γ), E=low; calculated astrophysical reaction rates. Shell model approach.

NUCLEAR STRUCTURE 46Cr; calculated levels, J, π, spectroscopic factors. Shell model.

doi: 10.1016/S0375-9474(03)00870-4


2003MA02     Phys.Rev. C 67, 014311 (2003)

P.F.Mantica, A.C.Morton, B.A.Brown, A.D.Davies, T.Glasmacher, D.E.Groh, S.N.Liddick, D.J.Morrissey, W.F.Mueller, H.Schatz, A.Stolz, S.L.Tabor, M.Honma, M.Horoi, T.Otsuka

β decay studies of the neutron-rich 56-58V isotopes

RADIOACTIVITY 56,57,58V(β-) [from Be(86Kr, X)]; measured Eγ, Iγ, βγ-, γγ-coin, T1/2; deduced log ft. 56,57,58Cr deduced levels, J, π. Systematics in neighboring isotones discussed. Comparison with model predictions.

doi: 10.1103/PhysRevC.67.014311
Data from this article have been entered in the XUNDL database. For more information, click here.


2003MA56     Phys.Rev. C 68, 044311 (2003)

P.F.Mantica, B.A.Brown, A.D.Davies, T.Glasmacher, D.E.Groh, M.Horoi, S.N.Liddick, D.J.Morrissey, A.C.Morton, W.F.Mueller, H.Schatz, A.Stolz, S.L.Tabor

β-decay properties of 55, 56Ti

RADIOACTIVITY 55,56Ti(β-) [from Be(86Kr, X)]; measured β-delayed Eγ, Iγ, γγ-coin, T1/2; deduced β-branching ratios, role of spin-flip process. 55,56V deduced levels, feeding intensities. Comparisons with previous results, model predictions.

doi: 10.1103/PhysRevC.68.044311
Data from this article have been entered in the XUNDL database. For more information, click here.


2002HO03     Phys.Rev. C65, 027303 (2002)

M.Horoi, B.A.Brown, V.Zelevinsky

Applying the Exponential Convergence Method: Shell-model binding energies of 0f7/2 Nuclei Relative to 40Ca

NUCLEAR STRUCTURE 42,43Sc, 44,45Ti, 46,47V, 48,49Cr, 50,51Mn, 52,53Fe, 54,55Co, 56Ni; calculated ground-state energies, J, π. Exponential convergence method, comparison with data.

doi: 10.1103/PhysRevC.65.027303


2002HO14     Phys.Rev. C66, 015801 (2002)

M.Horoi, R.Jora, V.Zelevinsky, A.St.J.Murphy, R.N.Boyd, T.Rauscher

45V(p, γ) Thermonuclear Reaction Rate Relevant to 44Ti Production in Core-Collapse Supernovae: General Estimates and Shell Model Analysis

NUCLEAR REACTIONS 45V(p, γ), E ≈ 0.1-2 MeV; calculated astrophysical S-factors, reaction rate, resonance contributions. Shell model analysis.

doi: 10.1103/PhysRevC.66.015801


2002HO16     Phys.Rev. C66, 024319 (2002)

M.Horoi, A.Volya, V.Zelevinsky

Random interactions, isospin, and the ground states of odd-A and odd-odd nuclei

NUCLEAR STRUCTURE 20,21Ne, 21,22,23Na, 23,24,25Mg, 25,26,27Al, 27,28Si, 30P, 34Cl, 38K, 42Sc, 46V; calculated most probable spin, isospin quantum numbers for ground states. Random interaction model.

doi: 10.1103/PhysRevC.66.024319


2001HO27     Phys.Rev.Lett. 87, 062501 (2001)

M.Horoi, B.A.Brown, V.Zelevinsky

Random versus Realistic Interactions for Low-Lying Nuclear Spectra

doi: 10.1103/PhysRevLett.87.062501


1999HO05     Phys.Rev.Lett. 82, 2064 (1999)

M.Horoi, A.Volya, V.Zelevinsky

Chaotic Wave Functions and Exponential Convergence of Low-Lying Energy Eigenvalues

NUCLEAR STRUCTURE 48Cr, 51Sc; calculated levels, J, π; deduced model convergence features, truncation criteria. Shell model, quantum chaotic many-body dynamics.

doi: 10.1103/PhysRevLett.82.2064


1996ZE05     Phys.Rep. 276, 85 (1996)

V.Zelevinsky, B.A.Brown, N.Frazier, M.Horoi

The Nuclear Shell Model as a Testing Ground for Many-Body Quantum Chaos

doi: 10.1016/S0370-1573(96)00007-5


1995HO05     Phys.Rev.Lett. 74, 231 (1995)

M.Horoi, B.A.Brown

Toward a Consistent Description of Parity Nonconservation in A = 18-21 Nuclei

NUCLEAR STRUCTURE 18,19,20F, 21Ne; calculated parity nonconserving T=0, 1 matrix elements. Shell model.

doi: 10.1103/PhysRevLett.74.231


1995HO16     Phys.Rev.Lett. 74, 5194 (1995)

M.Horoi, V.Zelevinsky, B.A.Brown

Chaos vs Thermalization in the Nuclear Shell Model

doi: 10.1103/PhysRevLett.74.5194


1995ZE04     Phys.Lett. 350B, 141 (1995)

V.Zelevinsky, M.Horoi, B.A.Brown

Information Entropy, Chaos and Complexity of the Shell Model Eigenvectors

doi: 10.1016/0370-2693(95)00324-E


1994HO12     Phys.Rev. C50, 775 (1994)

M.Horoi, G.Clausnitzer, B.A.Brown, E.K.Warburton

New Calculations of the Parity Nonconservation Matrix Element for J(πT) 0+1, 0-1 Doublet in 14N

NUCLEAR STRUCTURE 14N; calculated levels, B(λ), isoscalar parity nonconserving matrix element. Shell model.

doi: 10.1103/PhysRevC.50.775


1994HO13     Phys.Rev. C50, R2274 (1994)

M.Horoi, B.A.Brown, V.Zelevinsky

Truncation Method for Shell Model Calculations

doi: 10.1103/PhysRevC.50.R2274


1994HO14     Phys.Rev. C50, 2392 (1994)

M.Horoi

Parity Mixed Doublets in A = 36 Nuclei

NUCLEAR STRUCTURE 36Cl, 36Ar; calculated levels, parity forbidden transitions γ CP, asymmetry. Different weak interactions, shell model with effective interactions.

doi: 10.1103/PhysRevC.50.2392


1994HO17     Phys.Rev. C50, 2834 (1994)

M.Horoi

Staggering of the Nuclear Charge Radii in a Superfluid Model with Good Particle Number

NUCLEAR STRUCTURE 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Sn; calculated mean squared charge radii with, without deformation, neutron, proton pairing energies. Superfluid model, monopole pairing type 4-body interaction.

doi: 10.1103/PhysRevC.50.2834


1993GU11     J.Phys.(London) G19, 2063 (1993)

R.K.Gupta, M.Horoi, A.Sandulescu, M.Greiner, W.Scheid

Cluster Preformation Probabilities and Fine-Structure Effects in Heavy-Cluster Decays using Folding Potentials

RADIOACTIVITY 221Fr, 225Ac, 221,222,223,224,226Ra(14C); calculated cluster decay width, Q, cluster preformation probability, other features. Double-folding potentials.

doi: 10.1088/0954-3899/19/12/011


1993HO14     Phys.Rev. C48, R522 (1993)

M.Horoi, G.Clausnitzer

Proposed New Experimental Case to Investigate the Weak Parity Nonconserving Couplings in 20F

NUCLEAR STRUCTURE 20,19F; calculated parity nonconserving matrix elements; deduced parity nonconserving asymmetry estimate, possible experiment.

doi: 10.1103/PhysRevC.48.R522


1992SA30     Int.J.Mod.Phys. E1, 379 (1992)

A.Sandulescu, R.K.Gupta, W.Greiner, F.Carstoiu, M.Horoi

Role of Cluster Deformations on Their Preformation Probabilities in Radioactive Cluster-Decay Studies

RADIOACTIVITY 230Th, 234,232U(24Ne); 222,224,226Ra(14C); 228Th(20O); 236Pu, 234U(28Mg); calculated cluster preformation probability, Gamow factors, WKB pentrabilities. Folded Michigan-3-Yukawa potential.

doi: 10.1142/S0218301392000199


1991BR28     Rev.Roum.Phys. 36, 135 (1991)

I.Brandus, F.Carstoiu, O.Dumitrescu, M.Horoi, F.Nichitiu

Multistep Direct and Compound Nuclear Reactions with Polarized Projectiles

NUCLEAR REACTIONS 13C, 15N(p, p), (polarized p, p), E ≤ 1.17 MeV; calculated σ(θ), analyzing power vs E. Double-folding interaction potential, multi-step direct compound nuclear reactions.


1991KN03     Phys.Rev. C44, 491 (1991)

N.Kniest, M.Horoi, O.Dumitrescu, G.Clausnitzer

Isovector Parity Mixing in 16O Investigated via the 15N(p(pol), α0)12C Resonance Reaction

NUCLEAR REACTIONS 15N(polarized p, α), E=resonance; analyzed data. 16O level deduced isovector parity mixing, α-decay features.

doi: 10.1103/PhysRevC.44.491


1990DU01     Phys.Rev. C41, 1462 (1990)

O.Dumitrescu, M.Horoi, F.Carstoiu, G.Stratan

Parity Nonconserving Asymmetries in Resonance Scattering and Nuclear Reactions Induced by Polarized Protons

NUCLEAR REACTIONS 13C(polarized p, p), E=1.13-1.17 MeV; 15N(polarized p, p), E=0.6-0.8 MeV; calculated σ(E), analyzing power vs E. 15N(p, α), E not given; calculated parity nonconserving analyzing power.

doi: 10.1103/PhysRevC.41.1462


1990DU03     Nuovo Cim. 103A, 653 (1990)

O.Dumitrescu, M.Horoi

An Enlarged Superfluid Model of Atomic Nucleus

NUCLEAR STRUCTURE 197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Pb; calculated isotope shifts, rms charge radii. 152Sm; calculated levels. Enlarged superfluid model.


1987AP02     Nucl.Phys. A470, 64 (1987)

M.Apostol, I.Bulboaca, F.Carstoiu, O.Dumitrescu, M.Horoi

Alpha-Like Four Nucleon Correlations in Superfluid Phases of Atomic Nuclei

NUCLEAR STRUCTURE 152Nd, 156Sm, 160Gd, 164Dy, 168Er, 176Hf, 180W, 184Os, 240Pu, 246Cf; calculated coupling strength constants, gap parameters, mass differences, enhancement factors. BCS approach.

doi: 10.1016/0375-9474(87)90120-5


1987AP03     Europhys.Lett. 4, 197 (1987)

M.Apostol, I.Bulboaca, F.Carstoiu, O.Dumitrescu, M.Horoi

Dynamical Alpha-Type Correlations in Deformed Superfluid Nuclei

NUCLEAR STRUCTURE 152Nd, 160Gd, 168Er, 176Hf, 184Os; calculated superfluidity enhancement factors, α-type correlation coefficients.


1987AP04     Rev.Roum.Phys. 32, 533 (1987)

M.Apostol, I.Bulboaca, F.Carstoiu, O.Dumitrescu, M.Horoi

Alpha-Like Four Nucleon Correlations in Superfluid Phases of Atomic Nuclei

NUCLEAR STRUCTURE 152Nd, 156Sm, 160Gd, 164Dy, 168Er, 176Hf, 180W, 184Os, 240Pu, 246Cf; calculated pairing, gap parameters, mass differences, superfluid enhancement factors. Four-nucleon correlations, BCS.


1986AP01     Rev.Roum.Phys. 31, 657 (1986)

M.Apostol, I.Bulboaca, F.Carstoiu, O.Dumitrescu, M.Horoi

α-Like Superfluid Phase in Heavy Nuclei

NUCLEAR STRUCTURE 132Sn, 136Te, 140Xe, 144Ba, 148Ce, 152Nd, 156Sm, 160Gd, 164Dy, 168Er, 172Yb, 176Hf, 180W, 184Os, 188Pt, 192Hg, 196Pb, 200Po, 204Rn; calculated α-aggregate separation energies, average mass defects, proton, neutron and α-like superfluidities. Superfluidity model.


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